University of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography
|
|
- Roland Foster
- 6 years ago
- Views:
Transcription
1 University of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography 3. The Art of OCT Dr. Gereon Hüttmann / 2009
2 System perspective (links clickable) Light sources Superluminescent diodes Semiconductor amplifiers Femtosecond lasers Beam delivery and probes Hand-held probe Catheter Ophthalmoscope Microscope OCT imaging engine Resolution Reference delay scanning Doppler/polarization/spectroscopy Detection Frequency domain Computer control Drive system Real-time display Data management Image & signal processing Motion reduction Speckle reduction Image enhancement Rendering algorithms
3 Optical Coherence Tomography Base Technology Applications devices Clinical Applications
4 The Four Families of OCT Sampling Parameter Spectrum SNR n S Coherence function SNR n l / z S c max Time multiplexed (point detector) Swept Source (OFDR) Demanding light source Phase Noise FFT necessary TD-OCT Demanding phase mod. Phase Noise Reduced SNR Space multiplexed (line detector) SD-OCT Good optics needed Limitations due to detector performance FFT necessary Linear OCT Limitations due to detector performance Limited z-range Reduced SNR
5 Time Domain OCT Faserkoppler Photodiode1 - Photodiode Bandpaßfilter Faserkoppler Phasenmodulator Photodiode2 Lichtquelle Gleichrichter Bandpaßfilter Gleichrichter Tiefpaßfilter Computer Probenarmoptik Tiefpaßfilter Probe Fiber optical interferometer -> stable, flexible Sophisticated signal processing -> measurement over 10 orders of magnitude
6 The Reference Delay Line Linear translated mirror Multipass translated mirror
7 Rotation based delay-line
8
9 Fiber Streching
10 Light sources for OCT Continuous sources SLD/LED/superfluorescent fibers, center wavelength; 800 nm (SLD), 1300 nm (SLD, LED), 1550 nm, (LED, fiber), power: 1 to 10 mw (c.w.) is sufficient, coherence length; 10 to 15 mm (typically), Pulsed lasers mode-locked Ti:Al2O3 (800 nm), 3 micron axial resolution (or less).
11 Superluminescent diodes (SLDs) Definition: broadband semiconductor light sources based on superluminescence (Acronym: SLD) Superluminescent diodes (also sometimes called superluminescence diodes or superluminescent LEDs) are optoelectronic semiconductor devices which are emitting broadband optical radiation based on superluminescence. They are similar to laser diodes, containing an electrically driven p-n junction and an optical waveguide, but lack optical feedback, so that no laser action can occur. Optical feedback, which could lead to the formation of cavity modes and thus to pronounced structures in the spectrum and/or to spectral narrowing, is suppressed by means of tilting the output facet relative to the waveguide, and can be suppressed further with anti-reflection coatings. Superluminescence: amplified spontaneous emission
12 TD-OCT Faserkoppler Photodiode1 - Phasenmodulator Photodiode2 Faserkoppler Lichtquelle Bandpaßfilter Gleichrichter Tiefpaßfilter Computer Probenarmoptik Probe
13 FD-OCT (Spectral Radar) Refenenz SLD Objekt FFT Spektrometer
14 Signals in FD-OCT I( k) I I 2 I I cos k z S R S R
15
16 Phase-resolved FDOCT Sarunic MV, Choma MA, Yang CH, et al. Instantaneous complex conjugate resolved spectral domain and swept-source OCT using 3x3 fiber coup OPTICS EXPRESS 13 (3): FEB
17 Removing the Depth Ambiguities
18 Das Spektrometer Linear image Sensor mit 1024 (1) Pixel, 8µx125µm (2) 180nm Spektralbereich Auflösung 0.1 nm Messtiefe 1 mm FWHM 4 µm 150 (3) A-Scans (4) pro Sekunde SNR = 108 db (7) (9)
19 Image Sensors Adressierungslogik Adressierungslogik A:Passiv Pixel CMOS Sensor Adressierungslogik B: Active Pixel CMOS Sensor C: CCD Sensor
20 Signal [electrons] Relative amplitude Spatial Resolution of the Detector CMOS-Sensor LIS pixel 518 pixel 519 pixel 520 1, , , , ,2 0 a) Lateral position of focus [µm] 0, Spatial frequency [cycles/pixel]
21 Roll-Off of the Sensitivity
22 Noise [elektrons] Noise performance of the Detector NMOS Hamamatsu 3904 Hamamatsu 3903 CMOS (LIS 1024) quantum noise limit E7 1E8 Average charge per pixel [elektrons]
23 Signalaufbereitung
24 Spectral Shaping of the Spectrum (White Adjust) Hanning window
25 Intensity [a.u] Amplitu Spectral Shaping of the Spectrum 4,0 3,5 3,0 Hanning window Tapered Cosine Multi gauss Noisy Hanning window Tapered Cosine Multi gauss Noisy 2,5 80 2,0 1,5 60 1,0 40 0,5 0, Wavelength [a.u] 20 0,86 0,88 0,90 0,92 0,94 0,96 0,98 1,00 Pathlengthdifference [mm] Hanning window Tapered cosine window Multi gauss
26 Transformation to k=2 /
27 Swept-Source OCT
28 Swept Soures for OCT Scanning sources tune narrow-width wavelength over entire spectrum, resolution similar to other sources, advantage that reference arm is not scanned, advantage that fast scanning is feasible.
29 Multimode Operation
30
31 Fourier Domain Mode Lock (FDLM) Dispersice Pulse Streching
32
33 Dispersion in the Interferometer
34 4 2 optical path lengths and chromatic dispersion 1 L c Probe Photodiode No additional optics
35 4 3 Optical Path Lengths and Chromatic Dispersion 1 n g d Probe d Photodiode Additional optics with n g = n - l dn/dl 1
36 4 4 Optical Path Lengths and Chromatic Dispersion Probe d Photodiode Correction in the reference arm
37 4 5 Optical Path Lengths and Chromatic Dispersion 1 2 c L ( c l D d ) 0 chr Probe d Photodiode Group velocity dispersion D chr = 1/c 0 dn g /dl 0
38 46 Optical Path Lengths and Chromatic Dispersion Probe d Photodiode Correction by introducing GVD in the reference arm
39 47 Conditions for Balancing the Optical Path and GVD Balancing of optical path length probe n g d i n g reference d i Balancing of group velocity dispersion probe D d D d chr i chr i reference
40 48 Group Index of Refraction and Group Velocity Dispersion at 1300 nm D Material n chr g [ps/nm/km] Air 1,00 0 Fused Silica 1,46 2,6 BK7 1,52-2,32 Water (20 C) 1,34-19,4 (37 C) 1,34 23,9 BaSF1 1,62-42,3 SF57 1,83-115,9 GRIN-Lens EG27 (NSG) 1,53-47,7 ZD-fiber n. m. 0 NZD-fiber (LEAF) n. m. -24,3
41 49 n p, n g D chr [psec/nm/ km] Chromatic Dispersion of Fused Silica 1,48 0 1,47 n g -200 Quarz 1, SF57 1,45 n p ,44 0,8 0,9 1 1,1 1,2 1,3 1,4 Wellenlänge [µm] ,8 0,9 1 1,1 1,2 1,3 1,4 Wellenlänge [µm]
42 index of refrection 50 OCT Endoscope graded index lense (GRIN) radius GRIN lense in mm CCD-camera scanner 3 mm 0 endoscope 270 mm length
43 51 Compensation of GVD Length of NZD-fiber [mm] NZD fibre length inside the reference = 1,15 m
44 52 Compensation of GVD Length of NZD-fiber [mm] NZD fibre length inside the reference = 1,15 m
45 Application Systems Galvanometerscanner Collimator Lens Beamsplitterplate Probe
46
47 Micromotor Endoscope Herz PR, Chen Y, Aguirre AD, et al. Micromotor endoscope catheter for in vivo, ultrahigh-resolution optical coherence tomography OPTICS LETTERS 29 (19): OCT
Optical coherence tomography
Optical coherence tomography Peter E. Andersen Optics and Plasma Research Department Risø National Laboratory E-mail peter.andersen@risoe.dk Outline Part I: Introduction to optical coherence tomography
More informationsome aspects of Optical Coherence Tomography
some aspects of Optical Coherence Tomography SSOM Lectures, Engelberg 17.3.2009 Ch. Meier 1 / 34 Contents 1. OCT - basic principles (Time Domain Frequency Domain) 2. Performance and limiting factors 3.
More informationIsolator-Free 840-nm Broadband SLEDs for High-Resolution OCT
Isolator-Free 840-nm Broadband SLEDs for High-Resolution OCT M. Duelk *, V. Laino, P. Navaretti, R. Rezzonico, C. Armistead, C. Vélez EXALOS AG, Wagistrasse 21, CH-8952 Schlieren, Switzerland ABSTRACT
More informationTemporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism
VI Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism Fang-Wen Sheu and Pei-Ling Luo Department of Applied Physics, National Chiayi University, Chiayi
More informationOCT Spectrometer Design Understanding roll-off to achieve the clearest images
OCT Spectrometer Design Understanding roll-off to achieve the clearest images Building a high-performance spectrometer for OCT imaging requires a deep understanding of the finer points of both OCT theory
More information7 CHAPTER 7: REFRACTIVE INDEX MEASUREMENTS WITH COMMON PATH PHASE SENSITIVE FDOCT SETUP
7 CHAPTER 7: REFRACTIVE INDEX MEASUREMENTS WITH COMMON PATH PHASE SENSITIVE FDOCT SETUP Abstract: In this chapter we describe the use of a common path phase sensitive FDOCT set up. The phase measurements
More informationIntegrated photonic circuit in silicon on insulator for Fourier domain optical coherence tomography
Integrated photonic circuit in silicon on insulator for Fourier domain optical coherence tomography Günay Yurtsever *,a, Pieter Dumon a, Wim Bogaerts a, Roel Baets a a Ghent University IMEC, Photonics
More informationSpectral domain optical coherence tomography with balanced detection using single line-scan camera and optical delay line
Spectral domain optical coherence tomography with balanced detection using single line-scan camera and optical delay line Min Gyu Hyeon, 1 Hyung-Jin Kim, 2 Beop-Min Kim, 1,2,4 and Tae Joong Eom 3,5 1 Department
More informationExternal cavities for controling spatial and spectral properties of SC lasers. J.P. Huignard TH-TRT
External cavities for controling spatial and spectral properties of SC lasers. J.P. Huignard TH-TRT Bright Er - Partners. WP 3 : External cavities approaches for high brightness. - RISOE TUD Dk - Institut
More informationContinuum White Light Generation. WhiteLase: High Power Ultrabroadband
Continuum White Light Generation WhiteLase: High Power Ultrabroadband Light Sources Technology Ultrafast Pulses + Fiber Laser + Non-linear PCF = Spectral broadening from 400nm to 2500nm Ultrafast Fiber
More informationRECENTLY, using near-field scanning optical
1 2 1 2 Theoretical and Experimental Study of Near-Field Beam Properties of High Power Laser Diodes W. D. Herzog, G. Ulu, B. B. Goldberg, and G. H. Vander Rhodes, M. S. Ünlü L. Brovelli, C. Harder Abstract
More informationExternal-Cavity Tapered Semiconductor Ring Lasers
External-Cavity Tapered Semiconductor Ring Lasers Frank Demaria Laser operation of a tapered semiconductor amplifier in a ring-oscillator configuration is presented. In first experiments, 1.75 W time-average
More informationHigh-Coherence Wavelength Swept Light Source
Kenichi Nakamura, Masaru Koshihara, Takanori Saitoh, Koji Kawakita [Summary] Optical technologies that have so far been restricted to the field of optical communications are now starting to be applied
More informationExamination Optoelectronic Communication Technology. April 11, Name: Student ID number: OCT1 1: OCT 2: OCT 3: OCT 4: Total: Grade:
Examination Optoelectronic Communication Technology April, 26 Name: Student ID number: OCT : OCT 2: OCT 3: OCT 4: Total: Grade: Declaration of Consent I hereby agree to have my exam results published on
More informationTheory and Applications of Frequency Domain Laser Ultrasonics
1st International Symposium on Laser Ultrasonics: Science, Technology and Applications July 16-18 2008, Montreal, Canada Theory and Applications of Frequency Domain Laser Ultrasonics Todd W. MURRAY 1,
More informationR. J. Jones Optical Sciences OPTI 511L Fall 2017
R. J. Jones Optical Sciences OPTI 511L Fall 2017 Semiconductor Lasers (2 weeks) Semiconductor (diode) lasers are by far the most widely used lasers today. Their small size and properties of the light output
More informationAxsun OCT Swept Laser and System
Axsun OCT Swept Laser and System Seungbum Woo, Applications Engineer Karen Scammell, Global Sales Director Bill Ahern, Director of Marketing, April. Outline 1. Optical Coherence Tomography (OCT) 2. Axsun
More informationLecture 6 Fiber Optical Communication Lecture 6, Slide 1
Lecture 6 Optical transmitters Photon processes in light matter interaction Lasers Lasing conditions The rate equations CW operation Modulation response Noise Light emitting diodes (LED) Power Modulation
More informationHigh brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh, C. Panja, P.T. Rudy, T. Stakelon and J.E.
QPC Lasers, Inc. 2007 SPIE Photonics West Paper: Mon Jan 22, 2007, 1:20 pm, LASE Conference 6456, Session 3 High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh,
More informationOptical Fibers p. 1 Basic Concepts p. 1 Step-Index Fibers p. 2 Graded-Index Fibers p. 4 Design and Fabrication p. 6 Silica Fibers p.
Preface p. xiii Optical Fibers p. 1 Basic Concepts p. 1 Step-Index Fibers p. 2 Graded-Index Fibers p. 4 Design and Fabrication p. 6 Silica Fibers p. 6 Plastic Optical Fibers p. 9 Microstructure Optical
More informationHeterodyne swept-source optical coherence tomography for complete complex conjugate ambiguity removal
Heterodyne swept-source optical coherence tomography for complete complex conjugate ambiguity removal Anjul Maheshwari, Michael A. Choma, Joseph A. Izatt Department of Biomedical Engineering, Duke University,
More informationOptics and Lasers. Matt Young. Including Fibers and Optical Waveguides
Matt Young Optics and Lasers Including Fibers and Optical Waveguides Fourth Revised Edition With 188 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents
More informationOptical Digital Transmission Systems. Xavier Fernando ADROIT Lab Ryerson University
Optical Digital Transmission Systems Xavier Fernando ADROIT Lab Ryerson University Overview In this section we cover point-to-point digital transmission link design issues (Ch8): Link power budget calculations
More informationSimultaneous acquisition of the real and imaginary components in Fourier domain optical coherence tomography using harmonic detection
Simultaneous acquisition of the real and imaginary components in Fourier domain optical coherence tomography using harmonic detection Andrei B. Vakhtin *, Daniel J. Kane and Kristen A. Peterson Southwest
More informationWavelength Stabilization of HPDL Array Fast-Axis Collimation Optic with integrated VHG
Wavelength Stabilization of HPDL Array Fast-Axis Collimation Optic with integrated VHG C. Schnitzler a, S. Hambuecker a, O. Ruebenach a, V. Sinhoff a, G. Steckman b, L. West b, C. Wessling c, D. Hoffmann
More informationTransmitting Light: Fiber-optic and Free-space Communications Holography
1 Lecture 9 Transmitting Light: Fiber-optic and Free-space Communications Holography 2 Wireless Phone Calls http://havilandtelconews.com/2011/10/the-reality-behind-wireless-networks/ 3 Undersea Cable and
More informationAbsorption: in an OF, the loss of Optical power, resulting from conversion of that power into heat.
Absorption: in an OF, the loss of Optical power, resulting from conversion of that power into heat. Scattering: The changes in direction of light confined within an OF, occurring due to imperfection in
More informationPhotonics and Fiber Optics
1 UNIT V Photonics and Fiber Optics Part-A 1. What is laser? LASER is the acronym for Light Amplification by Stimulated Emission of Radiation. The absorption and emission of light by materials has been
More informationVixar High Power Array Technology
Vixar High Power Array Technology I. Introduction VCSELs arrays emitting power ranging from 50mW to 10W have emerged as an important technology for applications within the consumer, industrial, automotive
More informationApplication Instruction 002. Superluminescent Light Emitting Diodes: Device Fundamentals and Reliability
I. Introduction II. III. IV. SLED Fundamentals SLED Temperature Performance SLED and Optical Feedback V. Operation Stability, Reliability and Life VI. Summary InPhenix, Inc., 25 N. Mines Road, Livermore,
More informationZ-LASER Optoelektronik GmbH Stemmer 3d Technologietag Useful information on Z-Lasers for Vision
Z-LASER Optoelektronik GmbH Stemmer 3d Technologietag - 24.2.2011 Useful information on Z-Lasers for Vision The Company Core Competences How to Build a Z-LASER Electronics and Modulation Wavelength and
More informationLaser Sources for Frequency-Domain Optical Coherence Tomography FD-OCT
Laser Sources for Frequency-Domain Optical Coherence Tomography FD-OCT Photonic Sensing Workshop SWISSLaser.Net Biel, 17. 9. 2009 Ch. Meier 1/ 20 SWISSLASER.NET Ch. Meier 17.09.09 Content 1. duction 2.
More informationSimultaneous Measurements for Tunable Laser Source Linewidth with Homodyne Detection
Simultaneous Measurements for Tunable Laser Source Linewidth with Homodyne Detection Adnan H. Ali Technical college / Baghdad- Iraq Tel: 96-4-770-794-8995 E-mail: Adnan_h_ali@yahoo.com Received: April
More informationBasic concepts. Optical Sources (b) Optical Sources (a) Requirements for light sources (b) Requirements for light sources (a)
Optical Sources (a) Optical Sources (b) The main light sources used with fibre optic systems are: Light-emitting diodes (LEDs) Semiconductor lasers (diode lasers) Fibre laser and other compact solid-state
More informationSupplementary Materials
Supplementary Materials In the supplementary materials of this paper we discuss some practical consideration for alignment of optical components to help unexperienced users to achieve a high performance
More informationLow Coherence Interferometry for the Inline Measurement of Translucent Multilayer Structures
Low Coherence Interferometry for the Inline Measurement of Translucent Multilayer Structures S. Hölters, C. Farkas, R. Fleige, A. Lenenbach, R. Noll, Aachen Abstract In a joint national project with industrial
More informationPulsed-source spectral-domain optical coherence tomography with reduced motion artifacts
Pulsed-source spectral-domain optical coherence tomography with reduced motion artifacts S. H. Yun, G. J. Tearney, J. F. de Boer, and B. E. Bouma Harvard Medical School and Wellman Center of Photomedicine,
More informationHigh stability multiplexed fibre interferometer and its application on absolute displacement measurement and on-line surface metrology
High stability multiplexed fibre interferometer and its application on absolute displacement measurement and on-line surface metrology Dejiao Lin, Xiangqian Jiang and Fang Xie Centre for Precision Technologies,
More information60 MHz A-line rate ultra-high speed Fourier-domain optical coherence tomography
60 MHz Aline rate ultrahigh speed Fourierdomain optical coherence tomography K. Ohbayashi a,b), D. Choi b), H. HiroOka b), H. Furukawa b), R. Yoshimura b), M. Nakanishi c), and K. Shimizu c) a Graduate
More informationDispersion measurement in optical fibres over the entire spectral range from 1.1 mm to 1.7 mm
15 February 2000 Ž. Optics Communications 175 2000 209 213 www.elsevier.comrlocateroptcom Dispersion measurement in optical fibres over the entire spectral range from 1.1 mm to 1.7 mm F. Koch ), S.V. Chernikov,
More informationPh 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS
Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS Diode Laser Characteristics I. BACKGROUND Beginning in the mid 1960 s, before the development of semiconductor diode lasers, physicists mostly
More informationHigh-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W
High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W Joachim Sacher, Richard Knispel, Sandra Stry Sacher Lasertechnik GmbH, Hannah Arendt Str. 3-7, D-3537 Marburg,
More informationHow to build an Er:fiber femtosecond laser
How to build an Er:fiber femtosecond laser Daniele Brida 17.02.2016 Konstanz Ultrafast laser Time domain : pulse train Frequency domain: comb 3 26.03.2016 Frequency comb laser Time domain : pulse train
More informationCharacteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy
Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy Qiyuan Song (M2) and Aoi Nakamura (B4) Abstracts: We theoretically and experimentally
More informationRing cavity tunable fiber laser with external transversely chirped Bragg grating
Ring cavity tunable fiber laser with external transversely chirped Bragg grating A. Ryasnyanskiy, V. Smirnov, L. Glebova, O. Mokhun, E. Rotari, A. Glebov and L. Glebov 2 OptiGrate, 562 South Econ Circle,
More informationTheoretical Approach. Why do we need ultra short technology?? INTRODUCTION:
Theoretical Approach Why do we need ultra short technology?? INTRODUCTION: Generating ultrashort laser pulses that last a few femtoseconds is a highly active area of research that is finding applications
More informationA novel tunable diode laser using volume holographic gratings
A novel tunable diode laser using volume holographic gratings Christophe Moser *, Lawrence Ho and Frank Havermeyer Ondax, Inc. 85 E. Duarte Road, Monrovia, CA 9116, USA ABSTRACT We have developed a self-aligned
More informationMode analysis of Oxide-Confined VCSELs using near-far field approaches
Annual report 998, Dept. of Optoelectronics, University of Ulm Mode analysis of Oxide-Confined VCSELs using near-far field approaches Safwat William Zaki Mahmoud We analyze the transverse mode structure
More informationComparison of FMCW-LiDAR system with optical- and electricaldomain swept light sources toward self-driving mobility application
P1 Napat J.Jitcharoenchai Comparison of FMCW-LiDAR system with optical- and electricaldomain swept light sources toward self-driving mobility application Napat J.Jitcharoenchai, Nobuhiko Nishiyama, Tomohiro
More informationOptical Amplifiers Photonics and Integrated Optics (ELEC-E3240) Zhipei Sun Photonics Group Department of Micro- and Nanosciences Aalto University
Photonics Group Department of Micro- and Nanosciences Aalto University Optical Amplifiers Photonics and Integrated Optics (ELEC-E3240) Zhipei Sun Last Lecture Topics Course introduction Ray optics & optical
More informationSpectral phase shaping for high resolution CARS spectroscopy around 3000 cm 1
Spectral phase shaping for high resolution CARS spectroscopy around 3 cm A.C.W. van Rhijn, S. Postma, J.P. Korterik, J.L. Herek, and H.L. Offerhaus Mesa + Research Institute for Nanotechnology, University
More informationBasics of INTERFEROMETRY
Basics of INTERFEROMETRY Second Edition P. HARIHARAN School ofphysics, Sydney, Australia University of Sydney CPi AMSTERDAM BOSTON HEIDELBERG LONDON NEW YORK OXFORD PARIS SAN DIEGO SAN FRANCISCO SINGAPORE
More informationContents. Acknowledgments. iii. 1 Structure and Function 1. 2 Optics of the Human Eye 3. 3 Visual Disorders and Major Eye Diseases 5
i Contents Acknowledgments iii 1 Structure and Function 1 2 Optics of the Human Eye 3 3 Visual Disorders and Major Eye Diseases 5 4 Introduction to Ophthalmic Diagnosis and Imaging 7 5 Determination of
More informationCHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT
CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT In this chapter, the experimental results for fine-tuning of the laser wavelength with an intracavity liquid crystal element
More informationOptical Characterization and Defect Inspection for 3D Stacked IC Technology
Minapad 2014, May 21 22th, Grenoble; France Optical Characterization and Defect Inspection for 3D Stacked IC Technology J.Ph.Piel, G.Fresquet, S.Perrot, Y.Randle, D.Lebellego, S.Petitgrand, G.Ribette FOGALE
More informationis a method of transmitting information from one place to another by sending light through an optical fiber. The light forms an electromagnetic
is a method of transmitting information from one place to another by sending light through an optical fiber. The light forms an electromagnetic carrier wave that is modulated to carry information. The
More informationReflective optics-based line-scanning. spectral domain optical coherence. tomography system
Reflective optics-based line-scanning spectral domain optical coherence tomography system Mohammad Abu Hana Mustafa Kamal A Thesis In the Department of Mechanical and Industrial Engineering Presented in
More informationActive mode-locking of miniature fiber Fabry-Perot laser (FFPL) in a ring cavity
Active mode-locking of miniature fiber Fabry-Perot laser (FFPL) in a ring cavity Shinji Yamashita (1)(2) and Kevin Hsu (3) (1) Dept. of Frontier Informatics, Graduate School of Frontier Sciences The University
More informationPicosecond Pulses for Test & Measurement
Picosecond Pulses for Test & Measurement White Paper PN 200-0100-00 Revision 1.1 September 2003 Calmar Optcom, Inc www.calamropt.com Overview Calmar s picosecond laser sources are actively mode-locked
More informationFiber-Optic Communication Systems
Fiber-Optic Communication Systems Second Edition GOVIND P. AGRAWAL The Institute of Optics University of Rochester Rochester, NY A WILEY-iNTERSCIENCE PUBLICATION JOHN WILEY & SONS, INC. NEW YORK / CHICHESTER
More informationA new picosecond Laser pulse generation method.
PULSE GATING : A new picosecond Laser pulse generation method. Picosecond lasers can be found in many fields of applications from research to industry. These lasers are very common in bio-photonics, non-linear
More informationSupercontinuum based mid-ir imaging
Supercontinuum based mid-ir imaging Nikola Prtljaga workshop, Munich, 30 June 2017 PAGE 1 workshop, Munich, 30 June 2017 Outline 1. Imaging system (Minerva Lite ) wavelength range: 3-5 µm, 2. Scanning
More informationOptical Delay Line Application Note
1 Optical Delay Line Application Note 1.1 General Optical delay lines system (ODL), incorporates a high performance lasers such as DFBs, optical modulators for high operation frequencies, photodiodes,
More informationTechnical Explanation for Displacement Sensors and Measurement Sensors
Technical Explanation for Sensors and Measurement Sensors CSM_e_LineWidth_TG_E_2_1 Introduction What Is a Sensor? A Sensor is a device that measures the distance between the sensor and an object by detecting
More informationtaccor Optional features Overview Turn-key GHz femtosecond laser
taccor Turn-key GHz femtosecond laser Self-locking and maintaining Stable and robust True hands off turn-key system Wavelength tunable Integrated pump laser Overview The taccor is a unique turn-key femtosecond
More informationLaser Diode. Photonic Network By Dr. M H Zaidi
Laser Diode Light emitters are a key element in any fiber optic system. This component converts the electrical signal into a corresponding light signal that can be injected into the fiber. The light emitter
More informationIntegrated disruptive components for 2µm fibre Lasers ISLA. 2 µm Sub-Picosecond Fiber Lasers
Integrated disruptive components for 2µm fibre Lasers ISLA 2 µm Sub-Picosecond Fiber Lasers Advantages: 2 - microns wavelength offers eye-safety potentially higher pulse energy and average power in single
More informationBN 1000 May Profile Optische Systeme GmbH Gauss Str. 11 D Karlsfeld / Germany. Tel Fax
BN 1000 May 2000 Profile Optische Systeme GmbH Gauss Str. 11 D - 85757 Karlsfeld / Germany Tel + 49 8131 5956-0 Fax + 49 8131 5956-99 info@profile-optsys.com www.profile-optsys.com Profile Inc. 87 Hibernia
More informationModule 12 : System Degradation and Power Penalty
Module 12 : System Degradation and Power Penalty Lecture : System Degradation and Power Penalty Objectives In this lecture you will learn the following Degradation during Propagation Modal Noise Dispersion
More information(51) Int Cl.: G01B 9/02 ( ) G01B 11/24 ( ) G01N 21/47 ( )
(19) (12) EUROPEAN PATENT APPLICATION (11) EP 1 939 581 A1 (43) Date of publication: 02.07.2008 Bulletin 2008/27 (21) Application number: 07405346.3 (51) Int Cl.: G01B 9/02 (2006.01) G01B 11/24 (2006.01)
More informationTesting with 40 GHz Laser Sources
Testing with 40 GHz Laser Sources White Paper PN 200-0500-00 Revision 1.1 January 2009 Calmar Laser, Inc www.calmarlaser.com Overview Calmar s 40 GHz fiber lasers are actively mode-locked fiber lasers.
More informationBasics of INTERFEROMETRY
Basics of INTERFEROMETRY P Hariharan CSIRO Division of Applied Sydney, Australia Physics ACADEMIC PRESS, INC. Harcourt Brace Jovanovich, Publishers Boston San Diego New York London Sydney Tokyo Toronto
More informationA Narrow-Band Tunable Diode Laser System with Grating Feedback
A Narrow-Band Tunable Diode Laser System with Grating Feedback S.P. Spirydovich Draft Abstract The description of diode laser was presented. The tuning laser system was built and aligned. The free run
More informationEvaluation of Scientific Solutions Liquid Crystal Fabry-Perot Etalon
Evaluation of Scientific Solutions Liquid Crystal Fabry-Perot Etalon Testing of the etalon was done using a frequency stabilized He-Ne laser. The beam from the laser was passed through a spatial filter
More informationPhotonics and Optical Communication Spring 2005
Photonics and Optical Communication Spring 2005 Final Exam Instructor: Dr. Dietmar Knipp, Assistant Professor of Electrical Engineering Name: Mat. -Nr.: Guidelines: Duration of the Final Exam: 2 hour You
More informationLMT F14. Cut in Three Dimensions. The Rowiak Laser Microtome: 3-D Cutting and Imaging
LMT F14 Cut in Three Dimensions The Rowiak Laser Microtome: 3-D Cutting and Imaging The Next Generation of Microtomes LMT F14 - Non-contact laser microtomy The Rowiak laser microtome LMT F14 is a multi-purpose
More informationS.R.Taplin, A. Gh.Podoleanu, D.J.Webb, D.A.Jackson AB STRACT. Keywords: fibre optic sensors, white light, channeled spectra, ccd, signal processing.
White-light displacement sensor incorporating signal analysis of channeled spectra S.R.Taplin, A. Gh.Podoleanu, D.J.Webb, D.A.Jackson Applied Optics Group, Physics Department, University of Kent, Canterbury,
More informationOptoelectronic Oscillator Topologies based on Resonant Tunneling Diode Fiber Optic Links
Optoelectronic Oscillator Topologies based on Resonant Tunneling Diode Fiber Optic Links Bruno Romeira* a, José M. L Figueiredo a, Kris Seunarine b, Charles N. Ironside b, a Department of Physics, CEOT,
More informationMoving from biomedical to industrial applications: OCT Enables Hi-Res ND Depth Analysis
Moving from biomedical to industrial applications: OCT Enables Hi-Res ND Depth Analysis Patrick Merken a,c, Hervé Copin a, Gunay Yurtsever b, Bob Grietens a a Xenics NV, Leuven, Belgium b UGENT, Ghent,
More informationShort Ring Cavity Swept Source Based on a Highly Reflective Chirped FBG
PHOTONIC SENSORS / Vol. 5, No. 3, 215: 251 256 Short Ring Cavity Swept Source Based on a Highly Reflective Chirped FBG Radu-Florin STANCU * and Adrian PODOLEANU Applied Optics Group, School of Physical
More informationHigh-power semiconductor lasers for applications requiring GHz linewidth source
High-power semiconductor lasers for applications requiring GHz linewidth source Ivan Divliansky* a, Vadim Smirnov b, George Venus a, Alex Gourevitch a, Leonid Glebov a a CREOL/The College of Optics and
More informationUS-Patent 5,867,512 US-Patent 6,297,066 Power and Stability High Powered Littman / Metcalf External Cavity Diode Laser http://www.sacher-laser.com How does our Laser achieve high stability? Initial State
More informationCONTENTS. Chapter 1 Wave Nature of Light 19
CONTENTS Chapter 1 Wave Nature of Light 19 1.1 Light Waves in a Homogeneous Medium 19 A. Plane Electromagnetic Wave 19 B. Maxwell's Wave Equation and Diverging Waves 22 Example 1.1.1 A diverging laser
More informationTapered Amplifiers. For Amplification of Seed Sources or for External Cavity Laser Setups. 750 nm to 1070 nm COHERENT.COM DILAS.
Tapered Amplifiers For Amplification of Seed Sources or for External Cavity Laser Setups 750 nm to 1070 nm COHERENT.COM DILAS.COM Welcome DILAS Semiconductor is now part of Coherent Inc. With operations
More informationLight Sources, Modulation, Transmitters and Receivers
Optical Fibres and Telecommunications Light Sources, Modulation, Transmitters and Receivers Introduction Previous section looked at Fibres. How is light generated in the first place? How is light modulated?
More informationSpatially Resolved Backscatter Ceilometer
Spatially Resolved Backscatter Ceilometer Design Team Hiba Fareed, Nicholas Paradiso, Evan Perillo, Michael Tahan Design Advisor Prof. Gregory Kowalski Sponsor, Spectral Sciences Inc. Steve Richstmeier,
More informationPulsed-source and swept-source spectral-domain optical coherence tomography with reduced motion artifacts
Pulsed-source and swept-source spectral-domain optical coherence tomography with reduced motion artifacts S. H. Yun, G. J. Tearney, J. F. de Boer, and B. E. Bouma Harvard Medical School and Wellman Center
More informationCharacterization of a fibre optic swept laser source at 1!m for optical coherence tomography imaging systems
Proc. SPIE vol.7889, Conf. on Optical Coherence Tomography and Coherence Domain Optical Methods in Biomedicine XIV, Photonics West 2011 (San Francisco, USA, Jan. 22-27, 2011), paper 7889-100 Characterization
More informationGabor fusion technique in a Talbot bands optical coherence tomography system
Gabor fusion technique in a Talbot bands optical coherence tomography system Petr Bouchal, Adrian Bradu, and Adrian Gh. Podoleanu Applied Optics Group, School of Physical Sciences, University of Kent,
More informationEYP-DFB BFY02-0x0x
102 26.06.2014 DATA SHEET Revision 1.02 26.06.2014 page 1 from 5 General Product Information Product Application 760 nm DFB Laser with hermetic Butterfly Housing Spectroscopy Monitor Diode, Thermoelectric
More informationGlaucoma Advanced, LAbel-free High resolution Automated OCT Diagnostics GALAHAD
Project Overview Glaucoma Advanced, LAbel-free High resolution Automated OCT Diagnostics GALAHAD Jul-2017 Presentation outline Project key facts Motivation Project objectives Project technology Photonic
More informationGaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm
GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm Clifford Frez 1, Kale J. Franz 1, Alexander Ksendzov, 1 Jianfeng Chen 2, Leon Sterengas 2, Gregory L. Belenky 2, Siamak
More informationLecture 10. Dielectric Waveguides and Optical Fibers
Lecture 10 Dielectric Waveguides and Optical Fibers Slab Waveguide, Modes, V-Number Modal, Material, and Waveguide Dispersions Step-Index Fiber, Multimode and Single Mode Fibers Numerical Aperture, Coupling
More informationDynamic Phase-Shifting Electronic Speckle Pattern Interferometer
Dynamic Phase-Shifting Electronic Speckle Pattern Interferometer Michael North Morris, James Millerd, Neal Brock, John Hayes and *Babak Saif 4D Technology Corporation, 3280 E. Hemisphere Loop Suite 146,
More informationPropagation, Dispersion and Measurement of sub-10 fs Pulses
Propagation, Dispersion and Measurement of sub-10 fs Pulses Table of Contents 1. Theory 2. Pulse propagation through various materials o Calculating the index of refraction Glass materials Air Index of
More informationBinocular retinal eye-tracking system Product Requirements Document C. Light Technologies, Inc.
Binocular retinal eye-tracking system Product Requirements Document C. Light Technologies, Inc. Document Number 00001 Revisions Level Date 5 12-12-2016 This is a computer-generated document. The electronic
More informationCitation for published version (APA): Nguyen, D. V. (2013). Integrated-optics-based optical coherence tomography
UvA-DARE (Digital Academic Repository) Integrated-optics-based optical coherence tomography Nguyen, Duc Link to publication Citation for published version (APA): Nguyen, D. V. (2013). Integrated-optics-based
More informationPixel-remapping waveguide addition to an internally sensed optical phased array
Pixel-remapping waveguide addition to an internally sensed optical phased array Paul G. Sibley 1,, Robert L. Ward 1,, Lyle E. Roberts 1,, Samuel P. Francis 1,, Simon Gross 3, Daniel A. Shaddock 1, 1 Space
More informationFrequency Noise Reduction of Integrated Laser Source with On-Chip Optical Feedback
MITSUBISHI ELECTRIC RESEARCH LABORATORIES http://www.merl.com Frequency Noise Reduction of Integrated Laser Source with On-Chip Optical Feedback Song, B.; Kojima, K.; Pina, S.; Koike-Akino, T.; Wang, B.;
More informationLuminous Equivalent of Radiation
Intensity vs λ Luminous Equivalent of Radiation When the spectral power (p(λ) for GaP-ZnO diode has a peak at 0.69µm) is combined with the eye-sensitivity curve a peak response at 0.65µm is obtained with
More information